Matthew's Asgn: Difference between revisions
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Btheredude (talk | contribs) No edit summary |
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[[File:RLcircuit.jpg]] |
[[File:RLcircuit.jpg]] |
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The Laplace transform for an inductor |
The Laplace transform for an inductor: |
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<math>\displaystyle\mathcal{L} \left\{f(t)\right\}</math> = <math>\ Ls + Li \,\!</math> |
<math>\displaystyle\mathcal{L} \left\{f(t)\right\}</math> = <math>\ Ls + Li \,\!</math> |
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The Laplace transform for a resistor |
The Laplace transform for a resistor: |
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<math>\displaystyle\mathcal{L} \left\{f(t)\right\}</math> = <math>\ R\,\!</math> |
<math>\displaystyle\mathcal{L} \left\{f(t)\right\}</math> = <math>\ R\,\!</math> |
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<math>\ 0 = -s/(s^2+w^2) + RI(s) + LsI(s) - Li \,\!</math> |
<math>\ 0 = -s/(s^2+w^2) + RI(s) + LsI(s) - Li \,\!</math> |
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A series of algebraic manipulations follows to come up with I(s): |
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<math>\ s/(s^2+w^2) = (R+Ls)I(s) + Li \,\!</math> |
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<math>\ I(s) = s/((s^2+w^2)(R+Ls)) - Li/(R+Ls) \,\!</math> |
Revision as of 16:09, 1 November 2010
I decided that I would attempt to perform a simple analysis of a series RL circuit, which could then be used to do a more complex analysis on a basic transformer. I have always had interest in electronics, and transformers are key to basic electronics.
I decided that i would do the analysis of a RL circuit with the variables instead of given values.
Given:
V(t)=
V(s)=
I(0)=i
The Laplace transform for an inductor:
=
The Laplace transform for a resistor:
=
Therefore the Resulting Equation for the system after applying the Laplace Transform:
A series of algebraic manipulations follows to come up with I(s):